Parallel Transport
المؤلف:
Do Carmo, M
المصدر:
Riemannian Geometry. Boston, MA: Birkhäuser, 1993.
الجزء والصفحة:
...
10-7-2021
1476
Parallel Transport
The notion of parallel transport on a manifold
makes precise the idea of translating a vector field
along a differentiable curve to attain a new vector field
which is parallel to
. More precisely, let
be a smooth manifold with affine connectionVector Bundle Connection
, let
be a differentiable curve from an interval
into
, and let
be a vector tangent to
at
for some
. A vector field
is said to be the parallel transport of
along
provided that
,
, is a vector field for which
.
Note that the use of the quantifier parallel in the above definition makes reference to the fact that a parallel transport
of a vector field
along a curve
is necessarily covariantly constant, i.e.,
satisfies
 |
(1)
|
for all
where, here,
denotes the unique covariant derivative of
associated to
.
A standard result in differential geometry is that, under the above hypotheses, parallel transports are unique.
In addition to the above definition, some literature defines parallel transport in a more function analytic way. Indeed, given an interval
and a point
, a parallel transport
of
along
is nothing more than a linear transformation
 |
(2)
|
which maps
to
. It is obvious that this transformation is invertible, its inverse being given simply by parallel transport along the reversed portion of
from
to
. The expression
has added benefit, too, because despite being defined intrinsically in terms of the affine connection
on
, it also provides a mechanism whereby one can recover a manifold's affine connection given a collection
of parallel vector fields along a curve
. In particular, if
and
, then
 |
(3)
|
where
is the desired vector field given by the connection
and where
.
REFERENCES:
Do Carmo, M. Riemannian Geometry. Boston, MA: Birkhäuser, 1993.
Spivak, M. A Comprehensive Introduction to Differential Geometry, Vol. 2, 3rd ed. Berkeley, CA: Publish or Perish Press, 1999.
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